Doppler Effect
This definition page has been automatically generated. You can help ExoDictionary by expanding, updating, or correcting it. |
This autostub has not yet had its initial copyediting proof and may contain significant formatting and even factual errors. You can improve Exodictionary by cleaning up the page markup and verifying that the definition is correct and then removing this tag. |
This autostub has not yet had its initial categorization proof and may be categorized incorrectly. You can improve Exodictionary by removing inappropriate categories and then removing this tag. |
Doppler Effect
</dt>
The change in frequency
with which energy reaches a receiver when the receiver and the energy source
are in motion relative to each other. Also called Doppler shift.
</dd>
In the case of sound, or any other wave motion where a real medium of
propagation exists (excepting, therefore, light and other electromagnetic
radiations) one must distinguish two principal cases: If the source is in
motion with speed v relative to a medium which propagates the waves in
question at speed c, then the resting observer receives waves emitted, with
actual frequency f as if they had a frequency f' given by the Doppler equation
case of the source receding from the observer, and the vice versa for the negative sign. If, on the other hand, the source is at rest relative to the propagating medium while the observer moves with speed v relative to the source,
case of observer approaching the source. For electromagnetic radiation, f/f ' = [1Missing Image:img src="SP7-d_files/minusplus.gif" (v/c)]/[1 � (v/c)] where the top signs represent the source receding from the observer and the bottom signs, approaching the observer. </dd>
References
This article is based on NASA's Dictionary of Technical Terms for Aerospace Use